The speed of light in media ‘A’ and ‘B’ are 2.0 × 1010 cm/s and 1.5 × 1010 cm/s respectively. A ray of light enters from the medium B to A at an incident angle ‘θ’. If the ray suffers total internal reflection, then
\(θ = sin^{-1} (\frac{3}{4})\)
\(θ > sin^{-1} (\frac{2}{3})\)
\(θ < sin^{-1} (\frac{3}{4})\)
\(θ > sin^{-1} (\frac{3}{4})\)
To solve the problem, we must understand the concept of total internal reflection and the physics behind it.
When a light ray attempts to move from a medium of higher refractive index to one of lower refractive index (from medium B to A in this case), total internal reflection occurs if the angle of incidence is greater than a certain critical angle.
Given:
We can calculate the refractive indices of the media using the formula:
\(n = \frac{c}{v}\)
where \( n \) is the refractive index, \( c \) is the speed of light in a vacuum (\( 3.0 \times 10^{10} \) cm/s), and \( v \) is the speed of light in the medium.
Refractive index of medium A, \( n_A \):
\(n_A = \frac{3.0 \times 10^{10}}{2.0 \times 10^{10}} = 1.5\)
Refractive index of medium B, \( n_B \):
\(n_B = \frac{3.0 \times 10^{10}}{1.5 \times 10^{10}} = 2.0\)
Total internal reflection occurs when the angle of incidence is greater than the critical angle, which is determined by:
\(\sin \theta_c = \frac{n_A}{n_B} = \frac{1.5}{2} = 0.75\)
The critical angle, \( \theta_c \), is therefore:
\(\theta_c = \sin^{-1}(0.75)\)
Total internal reflection occurs if the angle of incidence \( \theta \) is greater than \( \theta_c \). Thus, the condition for total internal reflection is:
\(\theta > \sin^{-1}\left(\frac{3}{4}\right)\)
Hence, the correct option is:

A parallel beam of light travelling in air (refractive index \(1.0\)) is incident on a convex spherical glass surface of radius of curvature \(50 \, \text{cm}\). Refractive index of glass is \(1.5\). The rays converge to a point at a distance \(x \, \text{cm}\) from the centre of curvature of the spherical surface. The value of \(x\) is ___________.

